TY - JOUR

T1 - BC-Type Open SL(2,ℂ) Spin Chain

AU - Антоненко, Павел

AU - Деркачев, Сергей Эдуардович

AU - Валиневич, Павел

PY - 2026/1/7

Y1 - 2026/1/7

N2 - We diagonalize the B-element of monodromy matrix for noncompact open SL(2,C) spin chain with boundary interaction. The monodromy matrix is defined in terms of SL(2,C)L-operator and boundary K-matrix. The eigenfunctions of B-operator are constructed iteratively using raising Λ-operators. The key role in the calculations plays the Q-operator commuting with the B-operator. The main building blocks for Λ- and Q-operators are K-operator—the general solution of reflection equation and R-operator—the reduction of the general solution of the Yang–Baxter equation. Two types of the symmetry of eigenfunctions are established. The first kind is the invariance under permutations and reflections of spectral variables, or in other words, under the action of Weyl group of B and C root systems. The second kind is the symmetry with respect to transformation (s,g)→(1-s,1-g), where s is the spin variable and g is the parameter of K-matrix. We prove that obtained system of eigenfunctions is orthogonal and complete. The calculation of the scalar product of eigenfunctions is given in initial coordinate representation. We derive the Mellin–Barnes integral representation for eigenfunctions and use it to prove the completeness.

AB - We diagonalize the B-element of monodromy matrix for noncompact open SL(2,C) spin chain with boundary interaction. The monodromy matrix is defined in terms of SL(2,C)L-operator and boundary K-matrix. The eigenfunctions of B-operator are constructed iteratively using raising Λ-operators. The key role in the calculations plays the Q-operator commuting with the B-operator. The main building blocks for Λ- and Q-operators are K-operator—the general solution of reflection equation and R-operator—the reduction of the general solution of the Yang–Baxter equation. Two types of the symmetry of eigenfunctions are established. The first kind is the invariance under permutations and reflections of spectral variables, or in other words, under the action of Weyl group of B and C root systems. The second kind is the symmetry with respect to transformation (s,g)→(1-s,1-g), where s is the spin variable and g is the parameter of K-matrix. We prove that obtained system of eigenfunctions is orthogonal and complete. The calculation of the scalar product of eigenfunctions is given in initial coordinate representation. We derive the Mellin–Barnes integral representation for eigenfunctions and use it to prove the completeness.

UR - https://www.mendeley.com/catalogue/40ce7513-a4c5-3cbf-be59-6211f99a019d/

U2 - 10.1007/s00023-025-01653-0

DO - 10.1007/s00023-025-01653-0

M3 - Article

JO - Annales Henri Poincare

JF - Annales Henri Poincare

SN - 0018-0238

ER -